EP3114859A1 - Modélisation structurale de la réponse impulsionnelle relative à la tête - Google Patents

Modélisation structurale de la réponse impulsionnelle relative à la tête

Info

Publication number
EP3114859A1
EP3114859A1 EP15713262.2A EP15713262A EP3114859A1 EP 3114859 A1 EP3114859 A1 EP 3114859A1 EP 15713262 A EP15713262 A EP 15713262A EP 3114859 A1 EP3114859 A1 EP 3114859A1
Authority
EP
European Patent Office
Prior art keywords
pinna
model
torso
hrir
audio
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
EP15713262.2A
Other languages
German (de)
English (en)
Other versions
EP3114859B1 (fr
Inventor
C. Phillip Brown
Matthew Fellers
Regunathan Radhakrishnan
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Dolby Laboratories Licensing Corp
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Dolby Laboratories Licensing Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
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Publication date
Application filed by Dolby Laboratories Licensing Corp filed Critical Dolby Laboratories Licensing Corp
Publication of EP3114859A1 publication Critical patent/EP3114859A1/fr
Application granted granted Critical
Publication of EP3114859B1 publication Critical patent/EP3114859B1/fr
Active legal-status Critical Current
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Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04SSTEREOPHONIC SYSTEMS 
    • H04S7/00Indicating arrangements; Control arrangements, e.g. balance control
    • H04S7/30Control circuits for electronic adaptation of the sound field
    • H04S7/302Electronic adaptation of stereophonic sound system to listener position or orientation
    • H04S7/303Tracking of listener position or orientation
    • H04S7/304For headphones
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04SSTEREOPHONIC SYSTEMS 
    • H04S7/00Indicating arrangements; Control arrangements, e.g. balance control
    • H04S7/30Control circuits for electronic adaptation of the sound field
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04SSTEREOPHONIC SYSTEMS 
    • H04S1/00Two-channel systems
    • H04S1/007Two-channel systems in which the audio signals are in digital form
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04SSTEREOPHONIC SYSTEMS 
    • H04S2400/00Details of stereophonic systems covered by H04S but not provided for in its groups
    • H04S2400/11Positioning of individual sound objects, e.g. moving airplane, within a sound field
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04SSTEREOPHONIC SYSTEMS 
    • H04S2420/00Techniques used stereophonic systems covered by H04S but not provided for in its groups
    • H04S2420/01Enhancing the perception of the sound image or of the spatial distribution using head related transfer functions [HRTF's] or equivalents thereof, e.g. interaural time difference [ITD] or interaural level difference [ILD]

Definitions

  • FIG. 16 illustrates front/back tilt error as a function of the TILT parameter, under an embodiment.
  • HRTF CJiff (L, az) HRTF c (az)- HRTF c (-az)
  • the direction of b is thus dependent on a, which is dependent on the angle of elevation ⁇ ;
  • s is the unit vector in the direction of the source 1002 (which is the rectangular- to-polar conversion of the source elevation and azimuth);
  • d is the specified vector from the center 1008 of the torso 1004 to the ear 1006, where the position of the ear is specified with respect to the head sphere.
  • the vector d 2 is a vector that is orthogonal to d, and lies in the plane formed by s and d. It should be noted that a can be estimated as a function of ⁇ , according to Eq. 11:
  • the delay AT L p due to the filter was found to be 17 samples for a 44.1 kHz sample rate.
  • a diffusion network is applied to the torso reflection impulse response, conditioned on the elevation. For elevations near or below the horizon (elevation ⁇ 0 degrees) the signal will arrive tangentially (or near tangentially) to the torso and any acoustic energy that arrives at the ear will be heavily diffuse due to the acoustic scattering of the wave-front reflecting from the torso. This is modeled in the system with a diffusion network of which the degree of diffusion applied varies as a function of elevation as shown in FIG. 13.
  • FIG. 13 illustrates diffusion as a function of elevation for a diffusion network applied to a torso reflection impulse response, under an embodiment.
  • the average contains torso reflection components for frequencies below 2 kHz. Since the model contains a dedicated tool to apply torso reflection, the torso reflection components are removed from the front/back difference magnitude response. This may be accomplished by forcing the magnitude response to 0 dB below 2 kHz. A smooth cross-fade is applied between this frequency range, and the non-affected frequency range. The cross- fade is applied between 2 and 4 kHz. Likewise for elevations that would boost the gain above 0 dB at Nyquist, the gain is faded down such that the gain is 0 dB at Nyquist. This fade is applied between 20 to 22.05 kHz (for a sample rate of 44.1 kHz).
  • the structural HRIR model models the frequency location of pinna notches as function of elevation and azimuth.
  • the ILD and ITD cues are not sufficient to localize objects in 3D space.
  • the ITD and ILD values are identical as one varies the elevation from -45 to 225 degrees assuming an inter-aural coordinate system as described above. This set of points is usually referred to as the cone of confusion. To resolve two locations on the cone of confusion, one relies on the frequency locations of various pinna notches. The frequency location of the pinna notch is dependent on the source elevation at a given azimuth.
  • 'd' is the distance of the reflecting structure of pinna from the ear-canal entrance
  • 'c' is the speed of sound
  • 'f is frequency at which destructive interference happens resulting in a notch in the spectrum.

Abstract

L'invention concerne un procédé permettant de créer une réponse impulsionnelle relative à la tête (HRIR) destinée à être utilisée dans un rendu audio pour la lecture par le biais d'écouteurs, ledit procédé consistant à recevoir des paramètres de localisation pour un son comprenant l'azimut (az), l'élévation (el) et la portée (range) par rapport à la tête d'un auditeur; à appliquer un modèle de tête sphérique aux paramètres entrés d'azimut, d'élévation et de portée pour générer des valeurs HRIR binaurales; à calculer un modèle de pavillon au moyen des paramètres d'azimut et d'élévation à appliquer aux valeurs HRIR binaurales pour générer des valeurs HRIR modélisées de pavillon; à calculer un modèle de torse au moyen des paramètres d'azimut et d'élévation à appliquer aux valeurs HRIR modélisées du pavillon pour générer des valeurs HRIR modélisées de pavillon et de torse; et à calculer un modèle de champ proche au moyen des paramètres d'azimut et de portée à appliquer aux valeurs HRIR modélisées de pavillon et de torse pour générer des valeurs HRIR modélisées de pavillon, de torse et de champ proche.
EP15713262.2A 2014-03-06 2015-03-04 Modélisation structurale de la réponse impulsionnelle relative à la tête Active EP3114859B1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US201461948849P 2014-03-06 2014-03-06
PCT/US2015/018812 WO2015134658A1 (fr) 2014-03-06 2015-03-04 Modélisation structurale de la réponse impulsionnelle relative à la tête

Publications (2)

Publication Number Publication Date
EP3114859A1 true EP3114859A1 (fr) 2017-01-11
EP3114859B1 EP3114859B1 (fr) 2018-05-09

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Country Status (3)

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US (1) US10142761B2 (fr)
EP (1) EP3114859B1 (fr)
WO (1) WO2015134658A1 (fr)

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WO2015134658A1 (fr) 2015-09-11
US20170094440A1 (en) 2017-03-30
US10142761B2 (en) 2018-11-27
EP3114859B1 (fr) 2018-05-09

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